We consider the TRS containing the following rules:
a(x) | → | b(x) | (1) |
b(b(c(x))) | → | c(a(c(a(a(x))))) | (2) |
c(c(x)) | → | x | (3) |
The underlying signature is as follows:
{a/1, b/1, c/1}t0 | = | b(b(c(c(x109)))) |
→ | b(b(x109)) | |
= | t1 |
t0 | = | b(b(c(c(x109)))) |
→ | c(a(c(a(a(c(x109)))))) | |
→ | c(a(c(a(b(c(x109)))))) | |
→ | c(a(c(b(b(c(x109)))))) | |
→ | c(b(c(b(b(c(x109)))))) | |
→ | c(b(c(c(a(c(a(a(x109)))))))) | |
→ | c(b(c(c(a(c(a(b(x109)))))))) | |
→ | c(b(c(c(a(c(b(b(x109)))))))) | |
→ | c(b(c(c(b(c(b(b(x109)))))))) | |
→ | c(b(b(c(b(b(x109)))))) | |
→ | c(c(a(c(a(a(b(b(x109)))))))) | |
→ | c(c(a(c(a(b(b(b(x109)))))))) | |
→ | c(c(a(c(b(b(b(b(x109)))))))) | |
→ | c(c(b(c(b(b(b(b(x109)))))))) | |
→ | b(c(b(b(b(b(x109)))))) | |
= | t14 |